In this work, we focus on the medium property known as the
jet transverse momentum diffusion coefficient, \(\hat{q}\) ,
which describes the average transverse momentum, \(\langle k_{\perp }\rangle \) ,
acquired by a parton as it traverses a given length \(L\)  of QGP.
This transport coefficient is agnostic to the microscopic interactions that generate
the transverse diffusion, but rather characterizes the overall accumulated transverse momentum.
The transport coefficient \(\hat{q}\)  has been calculated
under certain approximations,[1]}, [2]}, [3]}, [4]}, [5]}, [6]}, [7]}, [8]} but in general involves nonperturbative
contributions that must be either computed on a lattice[9]}, [10]} or
extracted from experimental measurements.[11]}, [12]}, [13]}, [14]}
